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Introduction
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By examining the distributions of the estimates of the vector component of the wind stress, we show that they are also largest in February-April and smallest in July-September. Binning the vector components during these two intervals for each year, we computed the boundaries of the 95, 90 and 50 percentile intervals, and displayed in the figure to the right, their evolution since 1947. A dramatic decline in the 95 and 80% stress level was detected. In February to April of the 1960-80 interval, the magnitude of the stress during events that were less frequent than 5% was approximately 0.2 Pa. Since 2000 it has been 0.1 Pa. Summer statistics show a similar change. | (a) shows the boundaries of the stress intervals containing 95% (blue), 80% (green) and 50% (red) of the along LIS component stress estimates in February-April each year. (b) shows the same statistics but for the across LIS stress components. The data distribution evolution for the low wind July-September period are shown in (c) and (d) for the along and across Sound components respectively. |
We should be concerned that trends at a single station might
be the consequence of some local effect. Small movement of sensors or new
buildings can change airflow patterns for example. But the fact that the
reduction in wind speed was regional supports the interpretation that the
climate system is responsible for the change.
The record does not show much decadal-scale variation. The
trends in wind speed and stress show an increase from the 1940s to the 1960s,
and then an almost monotonic decrease. This variation is much more in-keeping
with the form of the Atlantic Multi-decadal Oscillation (AMO) that has been
described by Schlesinger and Ramankutty (1994). The AMO is manifest as
variation in the annual average sea surface temperature in the North Atlantic (30–65°N).
Trenberth and Shea (2006) showed that water temperature (positive AMO) led to
reduced storm activity and it has been linked empirically, and through models,
to several regional ocean and atmosphere trends. For example, above average
summer air temperatures in the eastern United States during positive AMO was
suggested by Enfield et al. (2001), and Goldenberg et al. (2001) found a
positive AMO anomaly was associated with increasing frequency of land-falling
hurricanes on the eastern seaboard.
The December AMO index from the NOAA ESRL analysis (black line) with the 95% bounds of the FMA along Sound stress distributions. The blue shows the lower bound and the red line is minus the upper bound. All three records have been standardized through division by the standard deviation. | This figure shows the AMO index developed by the NOAA earth Systems Research Laboratory (http://www.esrl.noaa.gov/psd/data/timeseries/AMO/) using satellite sea surface temperature maps. To simplify the graphics, we divide the index by the record standard deviation. The blue lines in (a) of the figure above show the upper and lower value of the along Sound stress component that are greater than 95% of the observations in a particular year. We repeat these lines in the figure to the left after dividing by the standard deviation and changing the sign of the upper (positive) bound. The similarity in the in the pattern of the curves is remarkable. Since the wind records only extend from 1947, less than a single oscillation has been captured. This correspondence can only be further investigated through models |
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A factor of two change in the stress should be expected to
have a significant effect on the ecosystems of the Sound. Reexamination of data
with the recognition of these long term changes have been occurring may bring
new insights to the understanding of the variability in LIS.
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